Faithful tensor generation #
The Burnside–Brauer theorem bounds the tensor powers needed to contain every irreducible complex representation of a finite group by the number of distinct values of a faithful character. The proof interpolates the indicator of the identity fibre of that character.
FDRep.exists_pos_finrank_hom_tensorPower proves the slightly stronger assertion that every
nonzero finite-dimensional representation has a nonzero map into one of these tensor powers.
For an irreducible source such a map is injective, so this is occurrence in an actual tensor
power, not merely membership in a span of characters. The zero-fold tensor power is included;
no positivity or irreducibility assumption on the faithful representation is needed.
The multiplicities mₙ = dim Hom_G(X, V^⊗n) are collected in the formal power series
FDRep.tensorMultiplicitySeries V X = ∑ₙ mₙ zⁿ. Since mₙ = |G|⁻¹ ∑_g χ_V(g)ⁿ χ_X(g⁻¹), it is the
finite sum of geometric series |G|⁻¹ ∑_g χ_X(g⁻¹) (1 - χ_V(g) z)⁻¹
(FDRep.tensorMultiplicitySeries_eq_characterFractions). Consequently it is a rational function:
multiplied by Q(z) = ∏_a (1 - a z), the product over the distinct character values a, it
becomes a polynomial of degree less than the number of values, and the multiplicities satisfy the
linear recurrence whose characteristic polynomial is ∏_a (T - a). These identities hold over
every field in which |G| is invertible, with the multiplicities read in that field.
For a faithful representation of positive dimension d, interpolating the identity fibre after
multiplying by Tᴮ shows that every window [B, B + r) of r consecutive exponents, r the
number of character values, contains a tensor power into which a given nonzero representation
maps nontrivially (FDRep.exists_mem_Ico_pos_finrank_hom_tensorPower). This gives the sharp
positive-power bound 1 ≤ n ≤ r and occurrence in arbitrarily large tensor powers, so that the
tensor-multiplicity series has infinitely many nonzero coefficients.
References #
- I. M. Isaacs, Character Theory of Finite Groups, Theorem 4.3.
- B. Steinberg, On the Burnside–Brauer–Steinberg theorem, arXiv:1409.7632, Introduction and Remark 1.
The construction uses Mathlib's Lagrange.basis and the finite-order trace criterion
Representation.char_eq_finrank_iff.
Character values are the image of the character on all group elements.
The coefficient expansion of the interpolator, including its constant term.
Evaluation of the interpolator detects the identity's character value.
The polynomial Q(z) = ∏_a (1 - a z) over the distinct character values a. It clears the
denominators of the tensor-multiplicity series; a zero character value contributes the factor
1.
Instances For
Character values may equally be enumerated over conjugacy classes.
The numerator N_X(z) = |G|⁻¹ ∑_g χ_X(g⁻¹) ∏_{a ≠ χ_V(g)} (1 - a z) of the
tensor-multiplicity series, the products running over the distinct character values of V.
Instances For
Coefficient–pairing interchange. Pairing χ_Vⁿ · P(χ_V) against χ_X computes the
combination ∑ⱼ P.coeff j · dim Hom_G(X, V^⊗(n + j)) of tensor multiplicities, for every
polynomial P.
The character-fraction identity. The tensor-multiplicity series is
|G|⁻¹ ∑_g χ_X(g⁻¹) (1 - χ_V(g) z)⁻¹, each factor inverted as a formal power series with
constant coefficient one; the n-th coefficient is |G|⁻¹ ∑_g χ_V(g)ⁿ χ_X(g⁻¹), with
χ_V(g)⁰ = 1 also when χ_V(g) = 0.
Rationality of the tensor-multiplicity series. Q(z) F_X(z) = N_X(z).
The linear recurrence of tensor multiplicities. If ∏_a (T - a) = ∑ⱼ cⱼ Tʲ, the product
running over the distinct character values of V, then ∑ⱼ cⱼ m_{n+j} = 0 for every n, where
mₙ = dim Hom_G(X, V^⊗n).
For a faithful complex representation the interpolator is the indicator of the identity.
Burnside–Brauer faithful tensor generation. Every nonzero finite-dimensional complex representation has a nonzero map into a tensor power of a faithful representation, with exponent strictly smaller than the number of its distinct character values. In particular every irreducible occurs among these tensor powers.
Burnside–Brauer, conjugacy-class bound. Every nonzero finite-dimensional complex representation has a nonzero map into a tensor power of a faithful representation, with exponent strictly smaller than the number of conjugacy classes.
Every irreducible complex representation embeds into one of the first tensor powers of a faithful representation.
Tensor generation in every window. For a faithful complex representation V of positive
dimension, every nonzero X has a nonzero map into V^⊗n for some n in each window
[B, B + r) of r consecutive exponents, where r is the number of character values of V.
The sharp positive-power bound. For a faithful complex representation V of positive
dimension, every nonzero X has a nonzero map into some positive tensor power V^⊗n with n at
most the number of character values of V. Positivity of dim V is necessary: the zero
representation of the trivial group is faithful, and all its positive tensor powers vanish.
Arbitrarily large tensor powers. For a faithful complex representation V of positive
dimension, every nonzero X has nonzero maps into arbitrarily large tensor powers of V, so the
tensor-multiplicity series of X has infinitely many nonzero coefficients.